Department of Chemistry, Christopher Ingold Laboratories, University College London, 20 Gordon Street, London, WC1H 0AJ, UK.
Phys Chem Chem Phys. 2010 Nov 7;12(41):13804-15. doi: 10.1039/c0cp00175a. Epub 2010 Sep 23.
First principles density functional theory (Perdew-Burke-Ernzerhof) calculations have been used to compute the hydration properties, aqueous-phase acid dissociation constants (pK(a)) and Gibbs free energies of formation of small polyphosphates in aqueous solution. The effect of the hydrated environment has been simulated through a hybrid microsolvation-continuum approach, where the phosphate species are simulated as microsolvated solutes, while the remainder of the bulk solvent is treated as a dielectric continuum using the COSMO solvation model. The solvation free energies of orthophosphates and pyrophosphates have been computed applying monomer and cluster thermodynamic cycles, and using the geometries optimised in the gas-phase as well as in the COSMO environment. The results indicate that the simple polarisable continuum or microsolvation-continuum models are unable to compute accurate free energies of solvation for charged species like phosphates. The calculation of the pK(a) shows that the computed values of acid dissociation constants are critically dependent on the number of water molecules n(H(2)O) included in the hydrated phosphate clusters. The optimal number n(H(2)O) is determined from the minimum value of the "incremental" water binding free energy associated with the process of adding a water molecule to a micro-solvated phosphate species. Analysis of the effect of n(H(2)O) on the free energies of orthophosphate condensation reactions shows that can vary by tenths of kcal mol(-1), depending on the particular choice of n(H(2)O) for the monomeric and dimeric species. We discuss a methodology for the determination of n(H(2)O); for the orthophosphates the "incremental" binding energy approach is used to determine n(H(2)O), whereas for the polyphosphates the number of explicit water molecules is simply equal to the effective charge of these anions. The application of this method to compute the free energy of formation of pyro- and tri-phosphates gives generally good agreement with the available experimental data.
采用第一性原理密度泛函理论(Perdew-Burke-Ernzerhof)计算方法,研究了水溶液中小聚磷酸盐的水合性质、水相酸离解常数(pKa)和生成吉布斯自由能。通过混合微溶剂化-连续体方法模拟水合环境的影响,将磷酸根物种模拟为微溶剂化溶质,而其余的体相溶剂则采用 COSMO 溶剂化模型作为介电连续体进行处理。采用单体和簇热力学循环计算正磷酸盐和焦磷酸盐的溶剂化自由能,并使用气相和 COSMO 环境中优化的几何形状。结果表明,简单的极化连续体或微溶剂化-连续体模型无法准确计算磷酸根等带电物种的溶剂化自由能。pKa 的计算表明,酸离解常数的计算值严重依赖于包含在水化磷酸根簇中的水分子数 n(H2O)。最佳水分子数 n(H2O)由与向微溶剂化磷酸根物种中添加一个水分子相关的“增量”水结合自由能的最小值确定。分析 n(H2O)对正磷酸盐缩合反应自由能的影响表明,取决于单体和二聚体物种中 n(H2O)的特定选择,n(H2O)的变化可以达到十分之几千卡摩尔-1。我们讨论了一种确定 n(H2O)的方法;对于正磷酸盐,采用“增量”结合能方法确定 n(H2O),而对于多磷酸盐,这些阴离子的有效电荷数即为明确水分子数。该方法用于计算焦磷酸盐和三磷酸盐的生成自由能,与现有实验数据吻合良好。